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Polarization and Light

Polarization refers to the separation of charge, either momentarily or permanently. [Pg.395]


R. A. Pasmanter, R. Samson, and A. Ben-Reuven. Molecular theory of optical polarization and light scattering in dielectric fluids. II. Extensions and applications. Phys. Rev. A, 74 1238-1250 (1976). [Pg.479]

Taptagapom, S., Saito, S. (1990). How display polarity and lighting conditions affect the pupil size of VDT operators. Ergonomics, 33, 201-208. [Pg.309]

Time and frequency domains are rigorously linked through a fourier transform (FT) operation and hence information gained in one domain can be readily interconverted into the other, as shown below for the polarization and light intensity in the medium. [Pg.346]

Figure 3 Scattering geometry for the usual measurement of depolarization ratios incident radiation is z-polarized and light scattered at right-angles is resolved for its y- and z-polarization components. Figure 3 Scattering geometry for the usual measurement of depolarization ratios incident radiation is z-polarized and light scattered at right-angles is resolved for its y- and z-polarization components.
In ellipsometry monochromatic light such as from a He-Ne laser, is passed through a polarizer, rotated by passing through a compensator before it impinges on the interface to be studied [142]. The reflected beam will be elliptically polarized and is measured by a polarization analyzer. In null ellipsometry, the polarizer, compensator, and analyzer are rotated to produce maximum extinction. The phase shift between the parallel and perpendicular components A and the ratio of the amplitudes of these components, tan are related to the polarizer and analyzer angles p and a, respectively. The changes in A and when a film is present can be related in an implicit form to the complex index of refraction and thickness of the film. [Pg.126]

Out of the five hydrodynamic modes, the polarized inelastic light scattering experiment can probe only the tliree modes represented by equation (A3.3.18), equation (A3.3.19) and equation (A3.3.20). The other two modes, which are in equation (A3.3.17), decouple from the density fluctuations diese are due to transverse... [Pg.723]

The Fresnel equations predict that reflexion changes the polarization of light, measurement of which fonns the basis of ellipsometry [128]. Although more sensitive than SAR, it is not possible to solve the equations linking the measured parameters with n and d. in closed fonn, and hence they cannot be solved unambiguously, although their product yielding v (equation C2.14.48) appears to be robust. [Pg.2838]

When light is incident on a material, the optical electric field E results in a polarization P of the material. The polarization can be expressed as the sum of the linear polarization and a nonlinear polarization P ... [Pg.256]

The sin 0 terms in Eqs. (10.25) and (10.26) arise from the consideration of polarized light. The light scattered by polarized incident light is also polarized in the same direction, so the term 1 + cos 0 in Eq. (10.30) describes the overall polarization of the scattered light. Before we lose sight of the individual contributions to this, it will be helpful to consider this polarization somewhat further. This is done in the following example. [Pg.673]

The intensity of the vertically polarized scattered light is proportional to sin 0 which, in polar coordinates, is described by a figure 8-shaped curve centered at the origin and having maximum values of 1 at 0 = 90°, Because 0 is symmetrical with respect to the z axis, this component of scattered light is described in three dimensions by a doughnut-shaped surface in which the hole has shrunk to a point - centered symmetrically in the xy plane. [Pg.674]

The all trans" stmcture in Figure 4.9(a) is not chiral as it has an inversion centre i. This is called a meso stmcture. Although each CFIFCFI3 group rotates the plane of plane-polarized light in one direction, the other group rotates it an equal amount in the opposite direction. The result is that there is no rotation of the plane of polarization and, as the presence of an inversion centre tells us, the molecule is achiral. [Pg.80]

Fig. 7. Fluorescence polarization (FP). (a) The formation of the large FITC—protein A—IgG complex which leads to a net increase in plane polarized light transmitted from the solution. Molecular weights of the protein A-FITC, IgG, and complex are ca 43,000, 150,000, and 343,000, respectively, (b) Detection of IgG by fluorescence polarization immunoassay using A, a laboratory fluorimeter where (O) represents AP = change in polarization, and B, a portable detection unit where (D) is —fiV = change in voltage (27). The field detector proved to be more sensitive than the fluorimeter. Fig. 7. Fluorescence polarization (FP). (a) The formation of the large FITC—protein A—IgG complex which leads to a net increase in plane polarized light transmitted from the solution. Molecular weights of the protein A-FITC, IgG, and complex are ca 43,000, 150,000, and 343,000, respectively, (b) Detection of IgG by fluorescence polarization immunoassay using A, a laboratory fluorimeter where (O) represents AP = change in polarization, and B, a portable detection unit where (D) is —fiV = change in voltage (27). The field detector proved to be more sensitive than the fluorimeter.
Fig. 12. A liquid crystal layer is radiant (middle) when placed between crossed polarizers and viewed against a light source. Fig. 12. A liquid crystal layer is radiant (middle) when placed between crossed polarizers and viewed against a light source.
Being only lightly polar and well below the Tg at common ambient temperatures the polymer is an excellent electrical insulator even at high frequencies. ... [Pg.587]

Polarization effects are another feature of Raman spectroscopy that improves the assignment of bands and enables the determination of molecular orientation. Analysis of the polarized and non-polarized bands of isotropic phases enables determination of the symmetry of the respective vibrations. For aligned molecules in crystals or at surfaces it is possible to measure the dependence of up to six independent Raman spectra on the polarization and direction of propagation of incident and scattered light relative to the molecular or crystal axes. [Pg.259]


See other pages where Polarization and Light is mentioned: [Pg.152]    [Pg.605]    [Pg.203]    [Pg.395]    [Pg.152]    [Pg.605]    [Pg.203]    [Pg.395]    [Pg.246]    [Pg.288]    [Pg.725]    [Pg.1195]    [Pg.1219]    [Pg.1222]    [Pg.1385]    [Pg.1878]    [Pg.1879]    [Pg.102]    [Pg.503]    [Pg.670]    [Pg.288]    [Pg.293]    [Pg.379]    [Pg.384]    [Pg.404]    [Pg.150]    [Pg.337]    [Pg.338]    [Pg.340]    [Pg.338]    [Pg.339]    [Pg.31]    [Pg.696]    [Pg.723]    [Pg.725]    [Pg.730]    [Pg.267]    [Pg.267]   


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Absorption and emission of polarized light

Absorption and emission spectroscopy with polarized light

Circularly and Elliptically Polarized Light

Electric and magnetic vectors in polarized light

Light Polarization

Partially polarized and unpolarized light

Plane-Polarized Light and 3-D Movies

Plane-Polarized Light and Handedness

Plane-Polarized Light and the Origin of Optical Rotation

Polarized Light and Optical Rotation

Polarized light

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